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# Title: Leibniz-Handschriften zur Mechanik: Dynamika LH 37, 5
# Folio 135v, page id 00068534:0266
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jam ut inveniatur centrum gravitatis
d seu recta Cd, et recra d7. resolvi
intelligatur hoc triangulum in tria triangula
isoselia, inter se aequalia FdG. GdE
Ed F. Et uuiue eorum ut GdE. area
er it tertia pars areae totius Tranguli R9
vel Aq. 243. Dividatur ergo area per 3. seu Rp. 9. fiet
fiet Rq 3f7. area Trianguli GdE.
4
s
as
quae alioquin etiam fit ex dluctu baside.
in altitudinem d3. ergo si Ag 27.
area basi Trianguli GdE. dividatur per
basin GE. 3. seu Rg. g. habebimus R4=
digidiam
pro da. quae si auferantur ex Fh. alti-
 8
in figura prima
tudine, quae est Rq 22 erit Ed. distantia centri gravitatis a puncto suspensionis a
Ry 27 R4
 etiam
ab distantia. ab. esto R Xerit in fig 1 bad. bEd.
+ + Rg 27. Ponderali Travitubit.
ergo Triangulum ex Rg 27. At in fig. 2.
4
travitabit x bad. quae componetur ex ba Rq 
et ad. Rq3. Erit summa bad. R4=
seu Rg vel Aq3
244
Euc ut est
admissa
Rg. 12. ad Rg. 4 ita erit, xhypothesi calculi
centri gravitatis,  Triangulum EFG in
fig. 3. ad idem in 4secunda fig 2da.
seu natio erit Rq  seu Ha _
seu D
Esto in fig. 4. idem Triangulum EFG. et linea
bai. quae in fig. 2 esto intelligatur rect angulum
IFG cujus longitudo bai. latitudo FG
fiat in fig.  Triangulum rectangutum,
cujus alti tndo bai. basiparallela in a.
sit F G. erit recta R ectangulum IFG. fig 5.
simile et aequale rectangulo 0 FG fig. 4.
repraesentabitque ejus pondus absolutum, in at
Trapezium ifGn repraesentabit potentiam
seu gravitationem Rectanguli oFG ex centro
bfiet totum Triangulum bin. F9. 5.
+ viceversa
facit 14..